Electromechanically
active ceramic materials, piezoelectrics and electrostrictors, provide
the backbone of a variety of consumer technologies. Gd- and Sm-doped
ceria are ion conducting ceramics, finding application in fuel cells,
oxygen sensors, and, potentially, as memristor materials. While optimal
design of ceria-based devices requires a thorough understanding of
their mechanical and electromechanical properties, reports of systematic
study of the effect of dopant concentration on the electromechanical
behavior of ceria-based ceramics are lacking. Here we report the longitudinal
electrostriction strain coefficient (
M
33
) of dense RE
x
Ce
1–
x
O
2–
x
/2
(
x
≤ 0.25) ceramic pellets, where RE = Gd or Sm, measured
under ambient conditions as a function of dopant concentration within
the frequency range
f
= 0.15–350 Hz and electric
field amplitude
E
≤ 0.5 MV/m. For >100
Hz, all ceramic pellets tested, independent of dopant concentration,
exhibit longitudinal electrostriction strain coefficient with magnitude
on the order of 10
–18
m
2
/V
2
. The quasi-static (
f
< 1 Hz) electrostriction
strain coefficient for undoped ceria is comparable in magnitude, while
introducing 5 mol % Gd or 5 mol % Sm produces an increase in
M
33
by up to 2 orders of magnitude. For
x
≤ 0.1 (Gd)–0.15 (Sm), the Debye-type relaxation
time constant (τ) is in the range 60–300 ms. The inverse
relationship between dopant concentration and quasi-static electrostrictive
strain parallels the anelasticity and ionic conductivity of Gd- and
Sm-doped ceria ceramics, indicating that electrostriction is partially
governed by ordering of vacancies and changes in local symmetry.